with \(B>A+1>1\)  which gives rise to the conventional hyperbolic
Pöschl-Teller potential [1]}
\(\tilde{V}^{(1)}_{con}(r)=[(A+1)A+B^{2}] {\rm cosech}^{2}r-B(2A+1) {\rm cosech}{r}\coth {r}+A^{2}\,.\) 
